US3190110A - Mechanical spike pulse filter for shock machine - Google Patents
Mechanical spike pulse filter for shock machine Download PDFInfo
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- US3190110A US3190110A US240182A US24018262A US3190110A US 3190110 A US3190110 A US 3190110A US 240182 A US240182 A US 240182A US 24018262 A US24018262 A US 24018262A US 3190110 A US3190110 A US 3190110A
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- 230000035939 shock Effects 0.000 title claims description 41
- 230000001133 acceleration Effects 0.000 claims description 18
- 238000012360 testing method Methods 0.000 claims description 10
- 238000001914 filtration Methods 0.000 claims description 7
- 230000000694 effects Effects 0.000 claims description 6
- 238000013461 design Methods 0.000 claims description 4
- 239000008188 pellet Substances 0.000 description 8
- 229910000831 Steel Inorganic materials 0.000 description 6
- 239000010959 steel Substances 0.000 description 6
- 239000013078 crystal Substances 0.000 description 4
- 238000012544 monitoring process Methods 0.000 description 4
- 239000007799 cork Substances 0.000 description 2
- 239000004568 cement Substances 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000001035 drying Methods 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012806 monitoring device Methods 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N3/00—Investigating strength properties of solid materials by application of mechanical stress
- G01N3/30—Investigating strength properties of solid materials by application of mechanical stress by applying a single impulsive force, e.g. by falling weight
- G01N3/303—Investigating strength properties of solid materials by application of mechanical stress by applying a single impulsive force, e.g. by falling weight generated only by free-falling weight
Definitions
- a very good square wave shock with a fast rise time is produced by dropping the carriage of such a drop tower on to an anvil from a predetermined height-
- a steel pin attached to the underside of the carriage strikes and penetrates a lead pellet placed on the anvil, and the dwell time is controlled by the depth .of penetration of the pin into the lead pellet.
- spike accelerations of many times the amplitude ofthe desired shock pulse are also produced.
- High frequency peak accelerations are generated by most shock machines Where square wave tests with fast rise'times are produced. These unwanted high. frequency peak accelerations are referred to as spikes.
- the square wave pulse is monitored and recorded with a low frequency accelerometer (strain gauge type) and amplifier system, the high frequency spikes will not be observed on the recording; however, this method does not reduce the effects of the spike acceleration on the specimen attached to the'carriage.
- a crystal accelerometer or other high frequency type monitoring device is used to record the shock pulse, thespike accelerations may be eliminated from the recorded output by using electronic filters, but this type of filtering does not reduce the spikes applied to the specimen.
- the spike acceleration amplitudes may be reduced by tapering the steel pin at the point of impact with the lead pellet, but this also is disadvantageous in that it increases the rise time.
- a purpose of the present invention is to minimize or eliminate the effects of the spike accelerations on a specimen while maintaining the desired square wave shock pattern.
- the present invention eliminates the effects of spike accelerationson a specimen by providing an isolator means attached to the carriage of a drop tower or the like.
- a plate, to which a specimen is attached, and the isolator are carried on the carriage of a typical drop tower such that the isolator filters most of the spikes from the adapter plate.
- the rise time of the pulse can be controlled by providing a tapered steel pin beneath the carriage which strikes and penetrates a lead pellet placed on an anvil.
- Another object of the invention is to provide a me- Patented June 22, 1965 ICC chanical filter for isolation of spike" accelerations produced by shock machines.
- a further object of the invention is to provide a true picture of a shock pulse by recording shock pulses with a crystal accelerometer without electronic filtering of the output signal.
- FIG. 1 illustrates a typical drop tower shock machine.
- FIG. 2 shows an adapter plate having a crystal accelerometer attached thereto.
- FIG. 3 shows an isolator which separates the adapter plate from the drop tower carriage.
- FIG. 4A illustrates a recording of a shock produced square wave pulse without any filtering.
- FIG. 4B shows .a recording of the pulse of FIG. using the mechanical filter of the present invention.
- FIGS. 5A and B show the pulses of FIGS. 4A and B with a gain of scope reduced by a factor of 4.
- FIGS. 6A and B also show the same pulses as in FIGS. 4A and B, but with the output signals from the accelerometer fed through an electronic filter- I
- the drop tower illustrated in FIG. 1 shows an 'anvil 10 at the base, a pair of guide rails 12 mounted on either side of the anvil, and a carriage 14 which guides on the rails.
- a release means 16 holds the carriage at its elevated position until'it is allowed to drop to the anvil.
- Carriage 14 carries a pin 18 attached to the underside thereof for piercing a pellet 17 of lead, for example, when the carriage is dropped.
- the upper surface of the carriage has an adapter plate 20 mounted. thereon for carrying a specimen to be tested. Between the carriage and adapter plate is mounted an isolator pad 22 of cork, or the like, and a highfrequency crystalaccelerometer 24,
- adapter plate 20 is attached to adapter plate 20.
- An electrical lead 25 connects accelerometer24 to a recorder 26 such as an oscilloscope and camera or the like.
- the adapter plate FIG. 2 and isolator FIG.'3 form the mechanical filter for the drop tower carriage.
- Plate 20 and isolator 22 may be attached to the carriage with a fast'drying cement, and a number of mounting holes may "be provided in the plate for attaching a specimen thereto.
- FIGS. 4-6 Recordings of square wave pulses using the aforementioned equipment (crystal accelerometer, oscilloscope and camera) are shown in FIGS. 4-6 for pulses with and without filtering.
- FIG. 4A shows a recording of a70g, 6 millisecond square wave pulse with the accelerometer attached to the carriage and with no filtering of any kind;
- FIG. 4B shows the same pulse with the accelerometer attached to the adapter plate and with isolator 22 between plate 20 and carriage 14.
- FIGS. 5A- and B also show the 70g, 6 millisecond pulse but with a gain of scope reduced by a factor of 4.
- the basic square wave shock is 70g while the spike acceleration amplitudes are 700g peak-to-peak and higher.
- FIGS. 6A and B are the same signals as in FIGS. 4A and B with the output signals from the accelerometer fed through a 5 kc. electronic filter.
- iUse of the present invention will isolate most spikes as shown by FIGS. 43 and 513 thus permitting better monitoring of specimens.
- a device asin claim 2 wherein said isolator pad is made from cork.
- a shock machine for producing square waves and the like having an anvil 'base, vertical guide rails and drop carriage upon which specimens to be shock'tested are mounted
- the improvement for eliminating the effects of spike accelerations on the test specimens comprisingz' e a (a) an isolator filter pad mounted on the top side of said drop carriage, (b) an'adapter plate mounted on .the top of said isolator pad for. attaching a test specimen thereto, (c) said isolator pad completely separating said adapter plate from said carriage, V I (d) a high frequency transmitting steel pin attached to the underside of said carriage .for strikingand penetrating. a lead pellet on the anvil base when the carriage 'is dropped,
- an adapter plate mounted-on top of. said isolator pad for attaching test specimens thereto
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- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)
Description
June 22, 1965 L. v. CRAYCRAFT 3,190,110
MECHANICAL SPIKE PULSE FILTER FOR SHOCK MACHINE Filed Nov. '26, 1962 2 Sheets-Sheet 1 MILLISECONDS FIG. 4A
MILLISECONDS FIG. 4B
LESTER V. CRAYCRAFT INVHVTOR.
Bydlhjm ATTORNEY June 22, 1965 v. CRAYCRAFT 3,190,l 10
MECHANICAL SPIKE PULSE FILTER FOR SHOCK MACHINE Filed Nov. 26; 1962 MILLISECONDS FIG. 5A
WITH
56o MECHANICAL 480 FILTER MILLISECONDS 'FI6.5B
2 Sheets-Sheet 2 ELECTRONIC FIL R 5KC I00 O 2 4 6 8 IO MILLISECONDS FIG. 6A
I40 MECHANICAL FILTER ELECTRONIC Fl R 5 KC LP MILLISECONDS FIG. 6B
LESTER V. CRAYCRAFT IN V EN TOR.
ATTORNEY United States Patent 3,190,110 MECHANICAL SPIKE PULSE FILTER FOR SHOCK MACHINE Lester V. Craycraft, Riverside, Calif., assignmto the United States of America asrepresented by the Secretary of the Navy Filed Nov. 26, 1962, Ser. No. 240,182 Claims. (CI. 73-12) (Granted under Title 35, US. Code 1952 see. 266) types of shock machines producing various types of shock pulses. To produce square wave shock pulses with a fast rise time of one millisecond or less a drop tower is normally used. A very good square wave shock with a fast rise time is produced by dropping the carriage of such a drop tower on to an anvil from a predetermined height- A steel pin attached to the underside of the carriage strikes and penetrates a lead pellet placed on the anvil, and the dwell time is controlled by the depth .of penetration of the pin into the lead pellet. However, at
the time of impact of the steel pin with the lead pellet, spike accelerations of many times the amplitude ofthe desired shock pulse are also produced. High frequency peak accelerations are generated by most shock machines Where square wave tests with fast rise'times are produced. These unwanted high. frequency peak accelerations are referred to as spikes.
If the square wave pulse is monitored and recorded with a low frequency accelerometer (strain gauge type) and amplifier system, the high frequency spikes will not be observed on the recording; however, this method does not reduce the effects of the spike acceleration on the specimen attached to the'carriage. Also, if a crystal accelerometer or other high frequency type monitoring device is used to record the shock pulse, thespike accelerations may be eliminated from the recorded output by using electronic filters, but this type of filtering does not reduce the spikes applied to the specimen. Further, the spike acceleration amplitudes may be reduced by tapering the steel pin at the point of impact with the lead pellet, but this also is disadvantageous in that it increases the rise time.
A purpose of the present invention is to minimize or eliminate the effects of the spike accelerations on a specimen while maintaining the desired square wave shock pattern. The present inventioneliminates the effects of spike accelerationson a specimen by providing an isolator means attached to the carriage of a drop tower or the like. A plate, to which a specimen is attached, and the isolator are carried on the carriage of a typical drop tower such that the isolator filters most of the spikes from the adapter plate. The rise time of the pulse can be controlled by providing a tapered steel pin beneath the carriage which strikes and penetrates a lead pellet placed on an anvil.
It is an object of the invention, therefore, to provide a mechanical filter for eliminating the effects of shock machine produced spike accelerations on a specimen being tested while maintaining a desired square wave shock pulse.
Another object of the invention is to provide a me- Patented June 22, 1965 ICC chanical filter for isolation of spike" accelerations produced by shock machines.
v A further object of the invention is to provide a true picture of a shock pulse by recording shock pulses with a crystal accelerometer without electronic filtering of the output signal.
Other objects and many of the attendant advantages of this invention will become readily appreciated as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings wherein:
FIG. 1 illustrates a typical drop tower shock machine.
FIG. 2 shows an adapter plate having a crystal accelerometer attached thereto.
FIG. 3 shows an isolator which separates the adapter plate from the drop tower carriage.
FIG. 4A illustrates a recording of a shock produced square wave pulse without any filtering.
FIG. 4B shows .a recording of the pulse of FIG. using the mechanical filter of the present invention.
FIGS. 5A and B show the pulses of FIGS. 4A and B with a gain of scope reduced by a factor of 4.
FIGS. 6A and B also show the same pulses as in FIGS. 4A and B, but with the output signals from the accelerometer fed through an electronic filter- I The drop tower illustrated in FIG. 1 shows an 'anvil 10 at the base, a pair of guide rails 12 mounted on either side of the anvil, anda carriage 14 which guides on the rails. A release means 16 holds the carriage at its elevated position until'it is allowed to drop to the anvil. Carriage 14 carries a pin 18 attached to the underside thereof for piercing a pellet 17 of lead, for example, when the carriage is dropped. The upper surface of the carriage has an adapter plate 20 mounted. thereon for carrying a specimen to be tested. Between the carriage and adapter plate is mounted an isolator pad 22 of cork, or the like, and a highfrequency crystalaccelerometer 24,
or the like, is attached to adapter plate 20. An electrical lead 25 connects accelerometer24 to a recorder 26 such as an oscilloscope and camera or the like. The adapter plate FIG. 2 and isolator FIG.'3 form the mechanical filter for the drop tower carriage. Plate 20 and isolator 22 may be attached to the carriage with a fast'drying cement, and a number of mounting holes may "be provided in the plate for attaching a specimen thereto.
In operation, when the carriage carrying a specimen is dropped the steel pin 18 will strike the lead pellet 17 and spike accelerations will be transmitted through pin 18 to carriage 14. Isolator 22, however, filters out most of the spikes from reaching the adapter plate to which the specimen is attached. e
Recordings of square wave pulses using the aforementioned equipment (crystal accelerometer, oscilloscope and camera) are shown in FIGS. 4-6 for pulses with and without filtering. FIG. 4A shows a recording of a70g, 6 millisecond square wave pulse with the accelerometer attached to the carriage and with no filtering of any kind; FIG. 4B shows the same pulse with the accelerometer attached to the adapter plate and with isolator 22 between plate 20 and carriage 14. FIGS. 5A- and B also show the 70g, 6 millisecond pulse but with a gain of scope reduced by a factor of 4. As shown in FIGS. 5A and B, the basic square wave shock is 70g while the spike acceleration amplitudes are 700g peak-to-peak and higher. FIGS. 6A and B are the same signals as in FIGS. 4A and B with the output signals from the accelerometer fed through a 5 kc. electronic filter.
From the foregoing it is apparent that with the present invention spike accelerations applied to a specimen are reduced by a factor of 10 to 1 when the specimen is subjected to square wave shocks.
Most military specifications .for square wave shocks specify a tolerance of ilO to 20% in the maximum amplitude of acceleration. Since most electronic packages are monitored for properoperation duringshock testsa component may pass the specified square wave shock but fire or trigger a circuit due to ;spikeaccelera-,
tions, which could result in specimen rejection and unwarranted delays in production or development of components. iUse of the present invention will isolate most spikes as shown by FIGS. 43 and 513 thus permitting better monitoring of specimens.
Obviously many modifications'and variations of' the present invention are possible in the light of the above It is therefore to be understood that within: the scope of the appended claims the invention maybe teachings.
practiced otherwise thanas specifically described.
What is claimed iszj V a 1. In a shock machine of the drop carriage design, for
v producing square waves and the like having an anvil base,
vertical guide rails and drop carriage upon which specimens to be shock tested are mounted, the improvements for eliminating the efiects of undesirable spike accelera-- men mounted thereon,
(d) said adapterpplate and isolator pad forming a mechanical filter for the drop carriage for filtering out unwantedlspike accelerations while 'maintaining the desired high rise time shock pulse pattern.
Yproducing square waves and the like havingan .anvil base, vertical guide rails and drop carriage'upon which specimens to be shock tested are mounted, the improvethe test specimens comprising'f (a an isolator filter pad mounted on the top side of said drop carriage, V
(b) an adapter plate mountedon the top of said isolator pad for attaching a test specimen thereto,
(c) said isolator pad completely separating said adapter plate from said carriage, v
(d) a high .frequency monitoring meansattached to fment for eliminating the elTects of spike accelerations on said adapted plate for recording shock wavestransmitted from said carriage and through said isolator to said adapter plate and any test specimen thereon when said carriage is dropped and strikes the anvil base of the shock machine; 7 (e) said padapter plate and isolator pad forming ;a
mechanical filter for the drop carriage for preventing-the unwanted spike accelerations from being transmitted from the carriage. to the specimen while maintaining the desired. high rise time shock pulse pattern.
DAVID SCHVONBERG, Examiner.
3. A device asin claim 2 wherein said isolator pad is made from cork.
4. In a shock machine {if the drop carriage design, for producing square waves and the like having an anvil 'base, vertical guide rails and drop carriage upon which specimens to be shock'tested are mounted, the improvement for eliminating the effects of spike accelerations on the test specimens comprisingz' e a (a) an isolator filter pad mounted on the top side of said drop carriage, (b) an'adapter plate mounted on .the top of said isolator pad for. attaching a test specimen thereto, (c) said isolator pad completely separating said adapter plate from said carriage, V I (d) a high frequency transmitting steel pin attached to the underside of said carriage .for strikingand penetrating. a lead pellet on the anvil base when the carriage 'is dropped,
(e) a monitoring means attached to said adapterplate' for recording shock waves transmitted from said can riage and throughsaid isolatorto said adapter. plate and any test-specimen thereon 'when said carriage. is dropped-and strikes'the anvil base of the shock machine V (f) said adapter plate and isolator pad forming a mechanical filter'for th e drop carriage for preventing 1 i V (b) an adapter plate mounted-on top of. said isolator pad for attaching test specimens thereto,
'(c) said isolator pad completely separating said adapter plate from said table, p
(d) monitoring means attached'to said adapter plate for :reeordingshock waves transmitted from said adapter plate and any test specimen thereon,
(e) said adapter plate and isolator pad forming. a mechanical filter for the dropcarriage for preventing unwanted spike accelerationsfrom being transmitted from .saidztable to the test specimen while maintaining the desired high rise time shock pulse pattern.
References Cited by the Examiner v UNITED STATES PATENTS 2,982,122 5/61 .Shatzet al. i 73 12 7 3,100,982 8/63 'Cutler 73 12 3,100,983 8/63. .De Vost 73 12 OTHER REFERENCES .Watertow'n; Mass, 4 pages. 1 p
. Journal Acoustical Soc. AM.,'vol. 28, No. 5, September 1956, article by Morrow .etal. pages 959-9 65.
RICHARD c. QUEISSER, Primary Examiner.
shock machine table through said isolator pad to said T Barry Products Bulletin 5 33, Barry Controls Inc., 7
Claims (1)
1. IN A SHOCK MACHINE OF THE DROP CARRIAGE DESIGN, FOR PRODUCING SQUARE WAVES AND THE LIKE HAVING AN ANVIL BASE, VERTICAL GUIDE RAILS AND DROP CARRIAGE UPON WHICH SPECIMENS TO BE SHOCK TESTED ARE MOUNTED, THE IMPROVEMENTS FOR ELIMINATING THE EFFECTS OF UNDESIRABLE SPIKE ACCELERATIONS ON THE TEST SPECIMENS COMPRISING: (A) AN ADAPTER PLATE MOUNTED ON SAID DROP CARRIAGE UPON WHICH A SPECIMEN TO BE TESTED CAN BE ATTACHED THERETO, (B) AN ISOLATOR FILTER PAD MOUNTED IN BETWEEN AND SEPARATING SAID ADAPTER PLATE FROM THE CARRIAGE, (C) AN ACCELEROMETER ATTACHED TO SAID ADAPTER PLATE THE OUTPUT OF WHICH IS USED FOR RECORDING THE SHOCK WAVE TRANSMITTED TO SAID ADAPTER PLATE AND ANY SPECIMEN MOUNTED THEREON, (D) SAID ADAPTER PLATE AND ISOLATOR PAD FORMING A MECHANICAL FILTER FOR THE DROP CARRIAGE FOR FILTERING OUT UNWANTED SPIKE ACCELERATION WHILE MAINTAINING THE DESIRED HIGH RISE TIME SHOCK PULSE PATTERN.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US240182A US3190110A (en) | 1962-11-26 | 1962-11-26 | Mechanical spike pulse filter for shock machine |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US240182A US3190110A (en) | 1962-11-26 | 1962-11-26 | Mechanical spike pulse filter for shock machine |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US3190110A true US3190110A (en) | 1965-06-22 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US240182A Expired - Lifetime US3190110A (en) | 1962-11-26 | 1962-11-26 | Mechanical spike pulse filter for shock machine |
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| US (1) | US3190110A (en) |
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3298222A (en) * | 1963-12-20 | 1967-01-17 | Gen Motors Corp | Device for measuring surface characteristics |
| US3339404A (en) * | 1963-11-26 | 1967-09-05 | George W Brooks | Lunar penetrometer |
| US3535912A (en) * | 1968-12-12 | 1970-10-27 | John T Muller | Apparatus for applying shock pulses |
| US3538743A (en) * | 1968-09-03 | 1970-11-10 | Avco Corp | Shock-testing machine control system |
| US3759085A (en) * | 1971-03-04 | 1973-09-18 | Massachusetts Inst Technology | Impact sensor and coder apparatus |
| US3960008A (en) * | 1974-12-12 | 1976-06-01 | Goble George G | Pile capacity testing means |
| DE4428765A1 (en) * | 1994-08-13 | 1996-02-15 | Thomas Franz Dipl In Schoesser | Impulse hammer used for measurement of structure-borne or airborne sound |
| DE19535686A1 (en) * | 1994-08-13 | 1997-03-27 | Thomas Franz Dipl In Schoesser | Device for inducing vibrations i.e. impulse hammer tester |
| US10590622B2 (en) * | 2016-07-18 | 2020-03-17 | Kunshan Construct Engineering Quality Testing Center | Drop hammer height adjusting device for high strain detection of pile foundation |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2982122A (en) * | 1957-05-29 | 1961-05-02 | Hughes Aircraft Co | Step function acceleration machine |
| US3100982A (en) * | 1960-12-28 | 1963-08-20 | Clarence W Cutler | Controlled shock or impact testing fixture |
| US3100983A (en) * | 1961-10-09 | 1963-08-20 | Vost Valmore F De | Dropable shock tester |
-
1962
- 1962-11-26 US US240182A patent/US3190110A/en not_active Expired - Lifetime
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2982122A (en) * | 1957-05-29 | 1961-05-02 | Hughes Aircraft Co | Step function acceleration machine |
| US3100982A (en) * | 1960-12-28 | 1963-08-20 | Clarence W Cutler | Controlled shock or impact testing fixture |
| US3100983A (en) * | 1961-10-09 | 1963-08-20 | Vost Valmore F De | Dropable shock tester |
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3339404A (en) * | 1963-11-26 | 1967-09-05 | George W Brooks | Lunar penetrometer |
| US3298222A (en) * | 1963-12-20 | 1967-01-17 | Gen Motors Corp | Device for measuring surface characteristics |
| US3538743A (en) * | 1968-09-03 | 1970-11-10 | Avco Corp | Shock-testing machine control system |
| US3535912A (en) * | 1968-12-12 | 1970-10-27 | John T Muller | Apparatus for applying shock pulses |
| US3759085A (en) * | 1971-03-04 | 1973-09-18 | Massachusetts Inst Technology | Impact sensor and coder apparatus |
| US3960008A (en) * | 1974-12-12 | 1976-06-01 | Goble George G | Pile capacity testing means |
| DE4428765A1 (en) * | 1994-08-13 | 1996-02-15 | Thomas Franz Dipl In Schoesser | Impulse hammer used for measurement of structure-borne or airborne sound |
| DE19535686A1 (en) * | 1994-08-13 | 1997-03-27 | Thomas Franz Dipl In Schoesser | Device for inducing vibrations i.e. impulse hammer tester |
| DE4428765C2 (en) * | 1994-08-13 | 1998-08-20 | Thomas Franz Dipl In Schoesser | Impact device |
| US10590622B2 (en) * | 2016-07-18 | 2020-03-17 | Kunshan Construct Engineering Quality Testing Center | Drop hammer height adjusting device for high strain detection of pile foundation |
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